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The Delft Sand, Clay & Rock Cutting Model, 2019a

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<strong>The</strong> <strong>Delft</strong> <strong>Sand</strong>, <strong>Clay</strong> & <strong>Rock</strong> <strong>Cutting</strong> <strong>Model</strong>.<br />

Wismer and Luth (1972A) and (1972B) investigated the inertia forces term I of the total cutting forces. <strong>The</strong><br />

following equation is derived:<br />

2 sin( )<br />

I s vc hi<br />

w<br />

sin( )<br />

(3-16)<br />

<strong>The</strong> cohesive and the adhesive forces C and A can be determined with soil mechanical experiments. For the<br />

cohesive and adhesive forces the following equations are valid:<br />

ch i w<br />

C sin( )<br />

ah b w<br />

A <br />

sin( )<br />

(3-17)<br />

(3-18)<br />

<strong>The</strong> gravitational force G (weight submerged) follows from:<br />

<br />

<br />

b i i<br />

G s w ghi<br />

w <br />

<br />

sin( ) sin( ) 2 sin( )<br />

<br />

sin( )<br />

<br />

h h sin( ) h cos( )<br />

<br />

<br />

<br />

<br />

<br />

(3-19)<br />

<strong>The</strong> gravitational force G (dry weight) follows from:<br />

<br />

sin( )<br />

h h sin( ) h cos( )<br />

<br />

<br />

<br />

<br />

b i i<br />

G s ghi w <br />

<br />

sin( ) sin( ) 2 sin( )<br />

<br />

(3-20)<br />

This is in accordance with the area that is used for the water pore pressure calculations in the case of water saturated<br />

sand (see Figure 6-7).<br />

3.4. <strong>The</strong> Curling Type.<br />

In some soils it is possible that the Curling Type of cutting mechanism occurs. This will happen when the layer<br />

cut is relatively thin and there is a force on the blade of which the magnitude depends on the blade height, like the<br />

adhesive force or the pore pressure force in the case of a cavitating cutting process. In soils like clay and loam, but<br />

also in rock under hyperbaric conditions this may occur. Figure 3-8 shows this Curling Type. <strong>The</strong> question now<br />

is, what is the effective blade height hb,m where the soil is in contact with the blade. To solve this problem, an<br />

additional equation is required. <strong>The</strong>re is only one equation available and that is the equilibrium equation of<br />

moments on the layer cut. Figure 3-9 shows the moments acting on the layer cut. In the case of clay, loam or<br />

hyperbaric rock, the contribution of gravity can be neglected.<br />

<strong>The</strong> equilibrium of moments when the gravity moment is neglected is:<br />

<br />

N W R N W R<br />

(3-21)<br />

1 1 1 2 2 2<br />

<strong>The</strong> arms of the 2 moments are:<br />

R<br />

h<br />

1 i<br />

1 , R2<br />

sin<br />

h<br />

<br />

2 b,m<br />

sin<br />

(3-22)<br />

This gives the equilibrium equation of moments on the layer cut:<br />

Page 80 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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